2022
DOI: 10.1103/physrevb.105.014202
|View full text |Cite
|
Sign up to set email alerts
|

Localization, PT symmetry breaking, and topological transitions in non-Hermitian quasicrystals

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
4
0

Year Published

2022
2022
2024
2024

Publication Types

Select...
5
1
1

Relationship

0
7

Authors

Journals

citations
Cited by 24 publications
(6 citation statements)
references
References 40 publications
0
4
0
Order By: Relevance
“…One can also tailor and control other higherorder topological phases exhibiting two-dimensional corner and three-dimensional hinge states by tuning the gain and loss or the periodic driving [172,177,178]. Recently, the study of non-Hermitian quasi-crystals has become a point of theoretical and experimental interest, given the immense body of work that has been dedicated to this particular topic [179][180][181][182][183][184]. The Floquet driving protocol enriches the topological features in non-Hermitian quasi-crystals revealing unique localization transitions.…”
Section: Floquet Engineering Of Non-hermitian Topological Phasesmentioning
confidence: 99%
“…One can also tailor and control other higherorder topological phases exhibiting two-dimensional corner and three-dimensional hinge states by tuning the gain and loss or the periodic driving [172,177,178]. Recently, the study of non-Hermitian quasi-crystals has become a point of theoretical and experimental interest, given the immense body of work that has been dedicated to this particular topic [179][180][181][182][183][184]. The Floquet driving protocol enriches the topological features in non-Hermitian quasi-crystals revealing unique localization transitions.…”
Section: Floquet Engineering Of Non-hermitian Topological Phasesmentioning
confidence: 99%
“…Non-Hermitian physics has attracted extensive attention, as non-Hermitian Hamiltonian can be used to explore the properties of open systems, quantum systems with gain and loss, as well as various classical systems [1][2][3][4][5][6][7][8][9][10][11]. In general, the energy band structure of non-Hermitian systems is complex, except for certain systems with pseudo-Hermiticity and parity-time (PT ) symmetry [12][13][14]. Additionally, non-Hermiticity realization is mainly based on nonreciprocal hoppings and on-site gain-loss [2,15,16].…”
Section: Introductionmentioning
confidence: 99%
“…Most works on the localized effect induced by the quasi-periodicity focus on the systems described by Hamiltonian. [17][18][19][20] In fact, discrete-time QW as a stroboscopic simulator of an effective Hamiltonian can be equivalent to a Floquet system, [21,22] in which both 0-energy states and π-energy states appear in the band gap. Meanwhile, mobility edges now are regarded as an energy threshold that distinguishes the local state from the extended state, [23][24][25][26][27][28][29] which was originally used in electronic systems to describe the migration properties of electrons in irregular crystalline potential fields.…”
Section: Introductionmentioning
confidence: 99%